The role of the top quark in many BSM models [1]}, [2]}, [3]}, [4]}, [5]}, [6]}
makes its interactions, in particular the electroweak gauge couplings,
sensitive probes that can be exploited by interpreting the differential \(\)  cross section in models with modified interactions of the top quark and the boson.
Extending the earlier analysis [7]}, where the inclusive cross section measurement was used, we consider an anomalous coupling Lagrangian [8]}

L = e u[  (\(C_{1,{V}}\) + 5 \(C_{1,{A}}\) ) + i  p \(m()\)  (\(C_{2,{V}}\) + i 5 \(C_{2,{A}}\) )
] v ,

which contains the neutral vector and axial-vector current couplings, \(C_{1,{V}}\)  and \(C_{1,{A}}\) , respectively.
The electroweak magnetic and electric dipole interaction couplings are denoted by \(C_{1,{V}}\)  and \(C_{1,{A}}\) , respectively, and
the four-momentum of the boson is denoted by \(p_\nu \) .
In total, there are four real parameters.
The current couplings are exactly predicted by the SM as

\(C_{1,{V}}\) SM=If3,-2Qf2\(\sin \theta _{}\cos \theta _{}\) = 0.2448 (52),
